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Abstracts Brochure - CERN

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THPCH — Poster Session 29-Jun-06 16:00 - 18:00<br />

Experiments were carried out with a magnetron<br />

gun having a cylindrical anode (70 mm in diameter): 1) with a smooth cathode (40 mm in diameter) and<br />

a modified cathode; 2) with four longitudinal seams; and 3) composed of eight copper rods (5 mm in diameter).<br />

Parameters of beams were studied and beam indentations were obtained. In the first case the beam formation occurs<br />

with a current of ∼40 A (at a cathode voltage of 40 kV) and an azimuthal uniformity of ± 5%. In the second case, at a<br />

field non-uniformity of ∼30%, the azimuthal non-uniformity is ∼15 A. In the third case, at a field non-uniformity of<br />

∼60% there occurs formation of eight separate beams having the form close to the half-ring and with a total current<br />

of ∼10A (at a cathode voltage of 30 kV). The beam current amplitude stability in all the cases was 2 . . . 5%.<br />

Investigation of Electron Beam Parameters in Magnetron Guns at Reduced Voltages<br />

The paper presents the results from investigations<br />

into the generation of electron beams V. Zakutin, A. Dovbnya, N.G. Reshetnyak (NSC/KIPT)<br />

and their parameters in magnetron guns<br />

with secondary-emission cathodes. The beam parameters were investigated for two cases. In the first case the<br />

magnetron gun cathode diameter was 40 mm, and the anode diameter was 70 mm. In the second case the magnetron<br />

gun cathode diameter was 2 mm, and the anode diameter was 7 mm. The experiments have shown that in the first<br />

case, with the anode diameter of 70 mm and the cathode voltage of 10 kV, the beam current was 7.5 A. The magnetic<br />

field value was 600 Oe. At a cathode voltage of 6 kV the beam current was 3A; however, then the amplitude and the<br />

triggering pulse decay rate should be increased to 100 kV/ms. In the second case at a pulse decay of ∼1200 kV/ms<br />

and a cathode voltage of 7 kV, the beam current was 2 A at a magnetic field value of ∼3000 Oe. The beam current as<br />

a function of the amplitude and the magnetic field distribution was studied.<br />

Experimental, Test and Research Beamlines at Fermilab<br />

Three new external beamlines are in operation<br />

or under development at Fermilab: 1)<br />

the Main Injector Particle Production (MIPP)<br />

beamline, 2) the Mucool Test Area (MTA)<br />

C. Johnstone, C.N. Brown, B. Choudhary, R.N. Coleman, M. De-<br />

Marteau, C.D. Moore, R. Raja, I. Rakhno, E. Ramberg (Fermilab)<br />

beamline, and 3) a new MTEST beamline for advanced detector work for high energy experiments and the ILC.<br />

The MIPP beamline is a secondary production beamline capable of producing well-characterized beams of protons,<br />

pions, and kaons from 5-120 GeV/c using 120 GeV/c protons from the Fermilab Main Injector. The second line is<br />

a new primary 400-MeV proton beamline derived from the 400 MeV proton Linac which will provide for precision<br />

measurements of Linac beam parameters in addition to a high-intensity primary test beam for development and<br />

verification of muon ionization cooling apparatus. A dual mode operation will also provide accurate, dispersionfree<br />

measurements of the Fermilab Linac beam properties with potential for diagnostic development. Installation is<br />

planned in 2007. Finally, a third beam is also under design to provide secondary beams at ultra-low - high energies,<br />

from ∼1 GeV/c to 90 GeV/c in addition to a primary 120-GeV proton mode of operation. It is anticipated that this<br />

last line will be installed in fall of 2006.<br />

443<br />

THPCH191<br />

THPCH192

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